2020
DOI: 10.1209/0295-5075/131/40004
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Barrier crossing in the presence of multi-exponential memory functions with unequal friction amplitudes and memory times

Abstract: We study the non-Markovian Langevin dynamics of a massive particle in a onedimensional double-well potential in the presence of multi-exponential memory by simulations. We consider memory functions as the sum of two or three exponentials with different friction amplitudes γi and different memory times τi and confirm the validity of a previously suggested heuristic formula for the mean first-passage time τMF P . Based on the heuristic formula, we derive a general scaling diagram that features a Markovian regime… Show more

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Cited by 12 publications
(11 citation statements)
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“…In fact, the values of and go down as moves to the respective start positions (i.e., as the folding and unfolding times become shorter). This reflects that memory effects particularly accelerate fast transitions ( 36 38 ).…”
Section: Resultsmentioning
confidence: 95%
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“…In fact, the values of and go down as moves to the respective start positions (i.e., as the folding and unfolding times become shorter). This reflects that memory effects particularly accelerate fast transitions ( 36 38 ).…”
Section: Resultsmentioning
confidence: 95%
“…1 , one obtains 6.8 ns, which is of the order of the longest memory time . This places the system in the so-called memory-acceleration regime, where memory effects are relevant and significantly accelerate barrier crossing ( 36 38 ).…”
Section: Resultsmentioning
confidence: 99%
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“…during chemical reactions [1][2][3], protein folding [4][5][6][7][8], nanomagnetic domain reversal [9], or even drug absorption [10]. As an important extension of the Kramers' problem, several studies considered a non-Markovian bath where memory effects influence the barrier crossing dynamics [11][12][13][14][15][16][17][18][19][20][21]. Such fluids are often found in biological environments but are also widespread in technical systems.…”
mentioning
confidence: 99%
“…Their motion is commonly described by the generalized Langevin equation [40] with nonequilibrium transient effects that markedly manifest themselves in presence of driving forces [41][42][43][44][45]. Although generalizations of Kramers rate theory to systems with longmemory friction have been developed in the past [46][47][48][49], apart from a few numerical works [28,29,[50][51][52], their predictions remain largely unexplored in experiments.…”
mentioning
confidence: 99%